• 제목/요약/키워드: plasma ion density

검색결과 257건 처리시간 0.031초

글로벌 모델에 의한 저온 고밀도 플루오로카본 플라즈마 특성의 공정변수 의존성 해석 (Analysis of Process Parameter dependency on the characteristics of high density fluoro carbon plasma using global model)

  • 이호준;태흥식
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 1999년도 추계학술대회 논문집 학회본부 C
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    • pp.879-881
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    • 1999
  • Radical and ion densities in a CF4 plasma have been calculated as a function of input power density. 9as pressure and feed gas flow rate using simple 0 dimensional global model. Fluorine atom is found to be the most abundant neutral particle. Highly fragmented species such as CF and CF+ become dominant neutral and ionic radical at the high power condition. As the pressure increases. ion density increases but ionization rate decreases due to the decrease in electron temperature. The fractional dissociation of CF4 feed gas decreases with pressure after increasing at the low pressure range. Electron density and temperature are almost independent of flow rate within calculation conditions studied. The fractional dissociation of CF4 monotonically decreases with flow rate. which results in increase in CF3 and decrease in CF density. The calculation results show that the SiO2 etch selectivity improvement correlates to the increase in the relative density of fluorocarbon ion and neutral radicals which has high C/F ratio.

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THE ION ACOUSTIC SOLITARY WAVES AND DOUBLE LAYERS IN THE SOLAR WIND PLASMA

  • Choi C.R.;Lee D.Y.;Kim Yong-Gi
    • Journal of Astronomy and Space Sciences
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    • 제23권3호
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    • pp.209-216
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    • 2006
  • Ion acoustic solitary wave in a plasma consisting of electrons and ions with an external magnetic field is reinvestigated using the Sagdeev's potential method. Although the Sagdeev potential has a singularity for n < 1, where n is the ion number density, we obtain new solitary wave solutions by expanding the Sagdeev potential up to ${\delta}n^4$ near n = 1. They are compressiv (rarefactive) waves and shock type solitary waves. These waves can exist all together as a superposed wave which may be used to explain what would be observed in the solar wind plasma. We compared our theoretical results with the data of the Freja satellite in the study of Wu et al. (1996). Also it is shown that these solitary waves propagate with a subsonic speed.

16Cr-10Ni-2Mo 스테인리스강의 정전류 실험에 의한 플라즈마 이온질화 온도 변수에 따른 부식 특성 (Corrosion Characteristics of 16Cr-10Ni-2Mo Stainless Steel with Plasma Ion Nitriding Temperatures by Galvanostatic Experiment)

  • 정상옥;김성종
    • 한국표면공학회지
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    • 제50권2호
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    • pp.91-97
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    • 2017
  • The aim of this paper is to investigate the characteristics of electrochemical corrosion with the plasma ion nitriding temperature for 16Cr-10Ni-2Mo stainless steel. The corrosion behavior was analyzed by means of galvanostatic experiment in natural seawater that applied various current density with plasma ion nitriding temperature parameters. In result of galvanostatic experiment, relatively less surface damage morphology and the less damage depth was observed at a nitrided temperature of $450^{\circ}C$ that measured the thickest nitrided layer(S-phase). On the other hand, the most damage depth and unified corrosion behavior presented at a temperature of $500^{\circ}C$.

High density plasma etching of novel dielectric thin films: $Ta_{2}O_{5}$ and $(Ba,Sr)TiO_{3}$

  • Cho, Hyun
    • 한국결정성장학회지
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    • 제11권5호
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    • pp.231-237
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    • 2001
  • Etch rates up to 120 nm/min for $Ta_{2}O_{5}$ were achieved in both $SF_{6}/Ar$ and $Cl_{2}/Ar$ discharges. The effect of ultraviolet (UV) light illumination during ICP etching on $Ta_{2}O_{5}$ etch rate in those plasma chemistries was examined and UV illumination was found to produce significant enhancements in $Ta_{2}O_{5}$ etch rates most likely due to photoassisted desorption of the etch products. The effects of ion flux, ion energy, and plasma composition on (Ba, Sr)$TiO_3$ etch rate were examined and maximum etch rate ~90 nm/min was achieved in $Cl_{2}/Ar$ ICP discharges while $CH_{4}/H_{2}/Ar$ chemistry produced extremely low etch rates (${\leq}10\;nm/min$) under all conditions.

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이중 주파수 전원의 용량성 결합 플라즈마 식각장비에서 전극하전에 의한 입사이온 에너지분포 변화연구 (Electrode Charging Effect on Ion Energy Distribution of Dual-Frequency Driven Capacitively Coupled Plasma Etcher)

  • 최명선;장윤창;이석환;김곤호
    • 반도체디스플레이기술학회지
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    • 제13권3호
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    • pp.39-43
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    • 2014
  • The effect of electrode charging on the ion energy distribution (IED) was investigated in the dual-frequency capacitively coupled plasma source which was powered of 100 MHz RF at the top electrode and 400 kHz bias on the bottom electrode. The charging property was analyzed with the distortion of the measured current and voltage waveforms. The capacitance and the resistance of electrode sheath can change the property of ion and electron charging on the electrode so it is sensitive to the plasma density which is controlled by the main power. The ion energy distribution was estimated by equivalent circuit model, being compared with the measured distribution obtained from the ion energy analyzer. Results show that the low frequency bias power changes effectively the low energy population of ion in the energy distribution.

Two-dimensional continuum modelling of an inductively coupled plasma reactor

  • Kim, Dong-Ho;Shung, Won-Young;Kim, Do-Hyun
    • 한국결정성장학회지
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    • 제10권2호
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    • pp.128-133
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    • 2000
  • Numerical analysis of the transport phenomena in an inductively coupled plasma reactor was conducted with two-dimensional axisymmetric model including the electromagnetic field model, electron and species density models. The spatial distribution of the charged species in the ion flux to the wafer have been calculated to examine the influence of the process conditions including antenna and reactor geometry. The antenna radius had a significant influence on the plasma state and axial ion flux distribution.

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고밀도 플라즈마 내에서의 plasma species의 변화 (The generation of nitrogen ion species in high-density plasma with HCD)

  • 김상권;김성완
    • 한국표면공학회:학술대회논문집
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    • 한국표면공학회 2009년도 춘계학술대회 논문집
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    • pp.234-234
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    • 2009
  • 고밀도 플라즈마 질화를 위해 장비 내에 보조 HCD (Hollow Cathode Discharge) 전극을 설치하여 고밀도의 플라즈마가 발휘되도록 장비를 구축하였다. 기존 bias 플라즈마 질화는 1-10Torr의 공정압력인데 반하여 $10^{-1}-10^{-2}$Torr의 비교적 고 진동에서 고밀도의 플라즈마를 발생시켰다. HCD 질화는 bias plasma 질화 공정의 플라즈마를 비교하면 가스 비의 영향이 매우 큰 것드로 관찰되었으며 기존에 발표된 플라즈마 질화 관련 모델과 비교하여 관찰된 플라즈마 내에서는 ion species가 실제 공정에서도 영향을 미치는 것을 알 수 있었다.

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Development of RF Ion Source for Neutral Beam Injector in Fusion Devices

  • 장두희;박민;김선호;정승호
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2013년도 제44회 동계 정기학술대회 초록집
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    • pp.550-551
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    • 2013
  • Large-area RF-driven ion source is being developed at Germany for the heating and current drive of ITER plasmas. Negative hydrogen (deuterium) ion sources are major components of neutral beam injection systems in future large-scale fusion experiments such as ITER and DEMO. RF ion sources for the production of positive hydrogen ions have been successfully developed at IPP (Max-Planck- Institute for Plasma Physics, Garching) for ASDEX-U and W7-AS neutral beam injection (NBI) systems. In recent, the first NBI system (NBI-1) has been developed successfully for the KSTAR. The first and second long-pulse ion sources (LPIS-1 and LPIS-2) of NBI-1 system consist of a magnetic bucket plasma generator with multi-pole cusp fields, filament heating structure, and a set of tetrode accelerators with circular apertures. There is a development plan of large-area RF ion source at KAERI to extract the positive ions, which can be used for the second NBI (NBI-2) system of KSTAR, and to extract the negative ions for future fusion devices such as ITER and K-DEMO. The large-area RF ion source consists of a driver region, including a helical antenna (6-turn copper tube with an outer diameter of 6 mm) and a discharge chamber (ceramic and/or quartz tubes with an inner diameter of 200 mm, a height of 150 mm, and a thickness of 8 mm), and an expansion region (magnetic bucket of prototype LPIS in the KAERI). RF power can be transferred up to 10 kW with a fixed frequency of 2 MHz through a matching circuit (auto- and manual-matching apparatus). Argon gas is commonly injected to the initial ignition of RF plasma discharge, and then hydrogen gas instead of argon gas is finally injected for the RF plasma sustainment. The uniformities of plasma density and electron temperature at the lowest area of expansion region (a distance of 300 mm from the driver region) are measured by using two electrostatic probes in the directions of short- and long-dimension of expansion region.

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Investigation of the Driving Frequency Effect on the RF-Driven Atmospheric Pressure Micro Dielectric Barrier Discharges

  • Bae, Hyowon;Lee, Jung Yeol;Lee, Hae June
    • Applied Science and Convergence Technology
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    • 제26권4호
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    • pp.74-78
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    • 2017
  • The discharge characteristics of the radio frequency (RF) surface dielectric barrier discharge have been simulated for the investigation of the ratio of the ion transit time to the RF period. From one-dimensional particle-in-cell (PIC) simulation for a planar dielectric barrier discharge (DBD), it was observed that the high-frequency driving voltage confines the ions in the plasma because of a shorter RF period than the ion transit time. For two-dimensional surface dielectric barrier discharges, a fluid simulation is performed to investigate the characteristics of RF discharges from 1 MHz to 40 MHz. The ratio of the peak density to the average density decreases with the increasing frequency, and the spatiotemporal discharge patterns change abruptly with the change in the ratio of ion transit time to the RF period.

오메가트론을 이용한 ECR 수소 플라프마 내의 이온 검출 (Detection of Ions in ECR $H_2$ Plasma Using Omegatron Mass Spectrometer)

  • 박정우;정희섭;김곤호;황기웅
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 1995년도 추계학술대회 논문집 학회본부
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    • pp.459-461
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    • 1995
  • An omegatron mass spectrometer was designed and fabricated. Experiments have been performed to demonstrate the instrument's operation in the ECR plasma device. By using this analyzer, mass spectra have been obtained in hydrogen plasmas, and typical results are presented. In the plasma omegatron, downstreaming plasma generated by ECR are entering the analyzer through a smsll floating aperture. We employ a biasing technique to reduce the ion velocity along the magnetic field and to keep the ions from drifting to the side pintos, and thus achieved improved ion collection and sensitivity. Mass spectra obtained show that main positive ion components are $H_3{^+}$ and $H_2{^+}$ with the density ratio of $H_2{^+}$ to $H_3{^+}$ $\simeq$ 0.2.

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